63,907 research outputs found
Confirming the LHC Higgs Discovery with WW
We investigate the prospects of observing a neutral Higgs boson decaying into
a pair of bosons (one real and the other virtual), followed by the
decays into or at the CERN Large Hadron Collider
(LHC). Assuming that the missing transverse energy comes solely from the
neutrino in decay, we can reconstruct the masses and then the Higgs
mass. At the LHC with a center of mass energy () of 8 TeV and an
integrated luminosity () of 25 fb, we can potentially establish a
signal. A discovery of for
TeV can be achieved with 6 fb. The discovery of
implies that the recently discovered new boson is a CP-even scalar
if its spin is zero. In addition, this channel will provide a good opportunity
to study the coupling
Higgs Boson Interference in
We study interference effects between resonant and nonresonant amplitudes for
the process at a backscattered
photon-photon collider. We show that a Higgs boson with > 200 GeV is
manifest as a resonant dip in the invariant mass spectrum and we
investigate its statistical significance.Comment: 8 pages (LaTeX) + 5 PostScript figures in accompanying file
(uuencoded), figures also available by fax upon request to
[email protected], UCLA/TEP/93/3
Gluon fusion contribution to W+W- + jet production
We describe the computation of the process that contributes
to the production of two -bosons and a jet at the CERN Large Hadron Collider
(LHC). While formally of next-to-next-to-leading order (NNLO) in QCD, this
process can be evaluated separately from the bulk of NNLO QCD corrections
because it is finite and gauge-invariant. It is also enhanced by the large
gluon flux and by selection cuts employed in the Higgs boson searches in the
decay channel , as was first pointed out by Binoth {\it et al.}
in the context of production. For cuts employed by the ATLAS
collaboration, we find that the gluon fusion contribution to
enhances the background by about ten percent and can lead to moderate
distortions of kinematic distributions which are instrumental for the ongoing
Higgs boson searches at the LHC. We also release a public code to compute the
NLO QCD corrections to this process, in the form of an add-on to the package
{\tt MCFM}.Comment: 13 pages, 4 figures, 3 table
Discovering the Higgs Bosons of Minimal Supersymmetry with Tau Leptons and a Bottom Quark
We investigate the prospects for the discovery at the CERN Large Hadron
Collider or at the Fermilab Tevatron of neutral Higgs bosons through the
channel where the Higgs are produced together with a single bottom quark and
the Higgs decays into a pair of tau leptons, . We work within the framework of the minimal
supersymmetric model. The dominant physics background from the production of
, (), ,
and is calculated with realistic acceptance cuts and efficiencies.
Promising results are found for the CP-odd pseudoscalar () and the heavier
CP-even scalar () Higgs bosons with masses up to one TeV.Comment: 14 pages, 7 figure
Single Charged Higgs production as a probe of CP violation at a Muon Collider
We consider single charged Higgs () production in association with a
boson at colliders, in the context of the general CP
violating Two Higgs Doublet Model (2HDM). We find that large cross-sections for
the processes are possible, and offer an
attractive way of producing at colliders. The difference
in the cross-sections for and may exceed 1000 fb, and this
represents a novel way of probing CP violation in the Higgs sector.Comment: 15 pages, LaTex, 6 figure
Searching for the Higgs Bosons of Minimal Supersymmetry with Muon Pairs and Bottom Quarks
The prospects for the discovery of neutral Higgs bosons (phi^0 = H^0, h^0,
A^0) produced with bottom quarks via Higgs decays into muon pairs (pp --> b
b-bar phi^0 --> b b-bar mu mu-bar +X) at the CERN LHC are investigated in the
minimal supersymmetric model. The complete physics background from the
production of b b-bar mu mu-bar, b b-bar W^+ W^- (including t t-bar) and jj mu
mu-bar, j = g, u, d, s, c in the Standard Model is calculated with realistic
acceptance cuts. This discovery mode has a simple production mechanism from gg
--> b b-bar phi^0 with its cross section proportional to 1/cos^2(beta) and
could provide an opportunity to measure tan(beta) and the b b-bar phi^0
couplings. In addition, we compare the associated discovery mode above with the
inclusive discovery channel pp --> phi^0 --> mu mu-bar +X. Promising results
are found for the CP-odd pseudoscalar (A^0) and the heavier CP-even scalar
(H^0) Higgs bosons for tan(beta) equivalent to v_2/v_1 >~ 14 and m_A,m_H <~ 325
GeV.Comment: 12 pages, REVTeX, 4 Figure
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